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Shadow Theory

Target-Relative Necessity of Completion: When Readout Loss Obstructs, and What a Sufficient Extension Must Retain

Active and inactive information loss

Jeremy RodgersSection 5 of 16Original PDF ↗Publication DOI ↗

Active and inactive information loss

We now sharpen the picture. Corollary 3.2 tells us that fiber variation of aQa_Q obstructs. But in practice one usually knows something more specific: one knows which source-level structure the readout has forgotten, and one wants to know whether that particular forgotten structure is what the target depends on. This is the distinction between information that is merely lost and information whose loss has consequences.

Definition 4.1 (Source relation and its target factorization).

Let r ⁣:S→Vr\colon S\to V be a map, called a source relation, thought of as recording some physically meaningful attribute of the reduced source state that the readout does not itself determine. We say that QQ factors through (p,r)(p,r) if there exists a map ΦQ ⁣:T×V⟶AQsuch thataQ(s)=ΦQ(p(s),r(s))for all s∈S.(7) \Phi_Q\colon T\times V\longrightarrow A_Q \qquad\text{such that}\qquad a_Q(s)=\Phi_Q\bigl(p(s),r(s)\bigr)\quad\text{for all }s\in S.\tag{7}

Equation (7) says that the readout value together with the relation value suffices to determine the correct answer. It is a modeling hypothesis about how much of the source the target actually consults; the interesting content lies in what one may then conclude.

Definition 4.2 (Activity and inactivity on a fiber).

Assume (7), and let t∈Tt\in T. The relation rr is active for QQ on the fiber FtF_t if there exist s0,s1∈Fts_0,s_1\in F_t with ΦQ(t,r(s0))≠ΦQ(t,r(s1)).(8) \Phi_Q\bigl(t,r(s_0)\bigr)\neq\Phi_Q\bigl(t,r(s_1)\bigr).\tag{8} It is inactive for QQ on FtF_t if no such pair exists, i.e. if the map ΦQ(t,⋅)\Phi_Q(t,\cdot) is constant on the realized set r(Ft)={ r(s):s∈Ft }⊆V.(9) r(F_t)=\{\, r(s) : s\in F_t \,\}\subseteq V .\tag{9} We say rr is globally inactive for QQ if it is inactive on every fiber.

Two features of Definition 4.2 carry the weight of the section, and both are easy to get wrong.

First, inactivity is a statement about the realized target values, not about rr. The relation rr may vary wildly across FtF_t , r(Ft)r(F_t) may be an enormous subset of VV , and rr may still be inactive for QQ on FtF_t, provided ΦQ(t,⋅)\Phi_Q(t,\cdot) happens to be constant on that subset. The readout has then forgotten a great deal, and none of it matters for QQ. This is the normal situation in effective descriptions and is not a pathology.

Second, activity is evaluated on the realized set r(Ft)r(F_t), not on all of VV. That ΦQ(t,⋅)\Phi_Q(t,\cdot) is nonconstant somewhere on VV is irrelevant if the source states in FtF_t never realize the values at which it varies. The obstruction concerns configurations that actually occur in the fiber.

Theorem 4.3 (Active loss obstructs).

Assume (7). If rr is active for QQ on some fiber FtF_{t}, then QQ is not exactly solvable from the readout pp.

Proof. Let s0,s1∈Fts_0,s_1\in F_{t} realize (8). Since s0,s1∈Fts_0,s_1\in F_{t} we have p(s0)=t=p(s1)p(s_0)=t=p(s_1). By (7), aQ(s0)=ΦQ(p(s0),r(s0))=ΦQ(t,r(s0))≠ΦQ(t,r(s1))=ΦQ(p(s1),r(s1))=aQ(s1).a_Q(s_0)=\Phi_Q\bigl(p(s_0),r(s_0)\bigr)=\Phi_Q\bigl(t,r(s_0)\bigr) \neq \Phi_Q\bigl(t,r(s_1)\bigr)=\Phi_Q\bigl(p(s_1),r(s_1)\bigr)=a_Q(s_1). Thus s0,s1s_0,s_1 satisfy the hypothesis (6) of Corollary 3.2, and QQ is not exactly solvable from pp. Indeed no map b ⁣:T→AQb\colon T\to A_Q is correct at both. ◻

Theorem 4.4 (Inactive loss does not obstruct).

Assume (7). If rr is globally inactive for QQ , that is, if for every t∈Tt\in T the map ΦQ(t,⋅)\Phi_Q(t,\cdot) is constant on the realized set r(Ft)r(F_t) , then QQ is exactly solvable from the readout pp. The unique readout-only solution is aˉQ(t)=ΦQ(t,vt)for any vt∈r(Ft).(10) \bar a_Q(t)=\Phi_Q\bigl(t,v_t\bigr) \qquad\text{for any } v_t\in r(F_t).\tag{10}

Proof. We verify condition (2) of Theorem 3.1. Fix t∈Tt\in T and let s,s′∈Fts,s'\in F_t. Then r(s),r(s′)∈r(Ft)r(s),r(s')\in r(F_t), and by global inactivity ΦQ(t,⋅)\Phi_Q(t,\cdot) is constant on r(Ft)r(F_t); hence ΦQ(t,r(s))=ΦQ(t,r(s′))\Phi_Q(t,r(s))=\Phi_Q(t,r(s')). Using (7) and p(s)=p(s′)=tp(s)=p(s')=t, aQ(s)=ΦQ(t,r(s))=ΦQ(t,r(s′))=aQ(s′).a_Q(s)=\Phi_Q\bigl(t,r(s)\bigr)=\Phi_Q\bigl(t,r(s')\bigr)=a_Q(s'). So aQa_Q is constant on FtF_t, for every tt. By Theorem 3.1, QQ is exactly solvable and the unique solution satisfies aˉQ(t)=aQ(s)\bar a_Q(t)=a_Q(s) for any s∈Fts\in F_t; since Ft≠∅F_t\neq\emptyset we may pick such an ss and set vt:=r(s)∈r(Ft)v_t:=r(s)\in r(F_t), giving (10). The right-hand side of (10) is independent of the choice of vt∈r(Ft)v_t\in r(F_t), again by constancy of ΦQ(t,⋅)\Phi_Q(t,\cdot) on r(Ft)r(F_t). ◻

Definition 4.5 (Structural versus consequential loss).

Let r ⁣:S→Vr\colon S\to V be a source relation that does not factor through pp; that is, rr is not constant on some fiber. We call this structural information loss: the readout genuinely fails to determine rr. If in addition rr is active for a target QQ on some fiber, we call the loss consequential for QQ, or target-active.

Theorem 4.3, Theorem 4.4 should be read with their standing hypothesis kept in view. Both presuppose that the nominated variable rr mediates the target, in the precise sense of (7): aQ(s)=ΦQ(p(s),r(s))a_Q(s)=\Phi_Q(p(s),r(s)). Relative to such an rr, the two theorems say that activity of rr is exactly the condition under which the loss of rr obstructs QQ , active loss obstructs, and globally inactive loss does not. This is a statement about the chosen mediating variable, not about information loss in the abstract, and it is only as sharp as the choice of rr.

The fully general criterion, carrying no such hypothesis, is the one already established in Theorem 3.1, Corollary 3.2: QQ is obstructed from the readout precisely when aQa_Q is nonconstant on some fiber of pp. Every statement about activity is a refinement of that criterion, obtained by localizing the fiber variation onto a particular mediating variable, and it adds diagnostic content , which forgotten structure is responsible , rather than logical strength.

With that scoping in place, the moral stands. Structural loss without activity is invisible to QQ; it is what makes coarse descriptions viable rather than defective. It is therefore not a theorem of this framework , and we do not assert , that every noninjective readout requires completion, nor that every lost source distinction must be restored. Whether a given loss must be repaired is a question one can only answer after nominating a target, and the answer may legitimately be no. The examples of Section 9, Section 10, Section 11 include both verdicts for the same readout.

Remark 4.6.

It is worth recording the logical relation between activity of rr and descent of rr. If rr itself descends along pp (is fiber-constant), then r(Ft)r(F_t) is a singleton for each tt and rr is automatically inactive for every target that factors through (p,r)(p,r); the loss is not merely inconsequential but nonexistent. The converse fails: rr can vary on fibers , structural loss , while being inactive for QQ. So activity implies structural loss, but structural loss does not imply activity, and it is precisely this asymmetry that forbids the inference from “noninjective” to “must be completed.”

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